2022/05/19 by Toloza, Julio H., Uribe, Alfredo · 1 citation
#34L15 (Primary) 34E10 #81Q05 #81Q10 (Secondary) #FOS: Mathematics #FOS: Physical sciences #Mathematical Physics (math-ph) #Spectral Theory (math.SP)
paper · doi:10.48550/arxiv.2205.09275
We consider the perturbed Stark operator Hqφ= -φ" + xφ+ q(x)φ, φ(0)=0, in L2(ℝ+), where q is a real-valued function that belongs to \mathfrakAr =\ q\inAr\capAC[0,∞) : q'\inAr\, where Ar = L2(ℝ+,(1+x)r dx) and r>1 is arbitrary but fixed. Let \λn(q)\n=1^ ∞ and \κn(q)\n=1^ ∞ be the spectrum and associated set of norming constants of Hq. Let \an\n=1^∞ be the zeros of the Airy function of the first kind, and let ωr:ℕ→ℝ be defined by the rule ωr(n) = n-1/3log1/2n if r∈(1,2) and ωr(n) = n-1/3 if r∈[2,∞). We prove that λn(q) = -an + π(-an)-1/2∫0^∞ Ai2(x+an)q(x)dx + O(n-1/3ωr2(n)) and κn(q) = - 2π(-an)-1/2∫0^∞ Ai(x+an)Ai'(x+an)q(x)dx + O(ωr3(n)), uniformly on bounded subsets of \mathfrakAr. In order to obtain these asymptotic formulas, we first show that λn:Ar→ℝ and κn:Ar→ℝ are real analytic maps.